Another main novelty is the construction of the
\(L_t^2\) -based temporal intermittent flows adapted to the structure of MHD,
which enables us to
control the stronger viscosity and resistivity \((-\Delta )^{{\alpha }_i}\) ,
\({\alpha }_i\ge 1\) , \(i=1,2\) .
We introduce the high temporal oscillations in the
velocity and magnetic flows.
Rather than the pointwise analysis in time,
we measure the solutions on average,
namely, in the space \(L^2_tL^2_x\) ,
which is in spirit close to the works [1]}, [2]}.
In particular, this new temporal intermittency
gains an extra almost 1D intermittency,
which enables us to
pass beyond the border line \({\alpha }_i =1\) 
and, more interestingly,
even to achieve all the exponents \({\alpha }_i\in [1,5/4)\) 
up to the sharp Lions exponent.
